On Friday, November 1, 2019 at 1:43:50 AM UTC-5, Alan Grayson wrote:
>
>
>
> On Friday, November 1, 2019 at 12:24:21 AM UTC-6, Philip Thrift wrote:
>>
>>
>>
>> On Thursday, October 31, 2019 at 4:33:29 PM UTC-5, Tomasz Rola wrote:
>>>
>>> On Thu, Oct 31, 2019 at 09:56:01AM -0700, Philip Thrift wrote: 
>>> > 
>>> > 
>>> > 
>>> http://backreaction.blogspot.com/2019/10/the-crisis-in-physics-is-not-only-about.html
>>>  
>>>
>>> Yeah. Interesting article and comments are worth a read, too. Perhaps 
>>> the problem she described stems from limits in human cognition. 
>>>
>>> quote: 
>>>
>>>    "But even if you don’t care what’s up with strings and multiverses, 
>>>    you should worry about what is happening here. The foundations of 
>>>    physics are the canary in the coal mine." 
>>>
>>> end quote 
>>>
>>> Indeed. I could not care less about strings and multiverses (unless I 
>>> can see a device making use of those theories), but I am a bit 
>>> worried. 
>>>
>>> -- 
>>> Regards, 
>>> Tomasz Rola 
>>>
>>> -- 
>>> ** A C programmer asked whether computer had Buddha's nature.      ** 
>>> ** As the answer, master did "rm -rif" on the programmer's home    ** 
>>> ** directory. And then the C programmer became enlightened...      ** 
>>> **                                                                 ** 
>>> ** Tomasz Rola          mailto:[email protected]     
>>
>>
>>
>>
>> There are all these projects, like "It from Qubit" (emergence of 
>> spacetime from quantum entanglement, Simons Foundation and Perimeter 
>> Institute) from 3 years ago, but they all seem to fizzle out and produce 
>> nothing.
>>
>> @philipthrift
>>
>
> They get more and more expensive, but many don't fizzle out; such as the 
> Kepler spacecraft which has found around 2000 planets, and many other 
> scientific spacecraft such as Galileo, Juno, Cassini, as well as the 
> several spacecraft that have mapped the CMBR in ever greater detail. I 
> could go on. Maybe she needs a cold shower. AG 
>



This has nothing to do with money for bigger and better instruments (bigger 
is better, right?).

It has to do with the fizzle out of fundamental theory.



>From the last conference:

The 2019 annual meeting of It from Qubit: Simons Collaboration on Quantum 
Fields, Gravity, and Information will be devoted to recent developments at 
the interface of fundamental physics and quantum information theory, 
spanning topics such as chaos and thermalization in many-body systems and 
their realization in quantum gravity; traversable wormholes and their 
information-theoretic implications; calculable lower-dimensional models of 
quantum gravity; the entanglement structure of semi-classical states in 
quantum gravity; complexity in field theory and gravity; the black-hole 
information puzzle; and applications of near-term quantum devices to 
problems in high-energy physics.

Abstracts

Matthew Headrick
Brandeis University

Bit Threads and Holographic Entropy Inequalities

Entanglement entropies in holographic theories as computed by the 
Ryu-Takayanagi formula are known to obey many inequalities beyond those 
required of general quantum states. Headrick will explain how these special 
properties can be understood in the language of bit threads and what they 
might imply for the entanglement structure of the underlying states.
 

Don Marolf
University of California, Santa Barbara

The Universal Structure of Holographic Quantum Codes

Don Marolf argues that the structure of holographic quantum codes is 
related to a simple splitting into two parts of the bulk gravitational path 
integrals. In particular, treating the bulk as an effective field theory 
means that we are given an effective Lagrangian LΛ associated with a 
cut-off energy scale Λ. We show that aspects of the code are then 
determined by classical computations involving LΛ, while the path integral 
over fluctuations below the scale Λ determines the states to be encoded. As 
a result, in each superselection sector, all such codes turn out to have 
flat entanglement spectrum up to corrections of order G (i.e., up to 
corrections of order G2 times the leading term, which is itself of order 
1/G). This statement holds for any LΛ, no matter what higher derivative 
terms it may contain. Marolf also comments on other applications of 
fixed-area states or more generally of states with fixed geometric entropy.
 

Vijay Balasubramanian
University of Pennsylvania

Quantum Complexity of Time Evolution with Chaotic Hamiltonians

Balasubramanian studies the quantum complexity of time evolution in large-N 
chaotic systems, with the SYK model as our main example. This complexity is 
expected to increase linearly for exponential time prior to saturating at 
its maximum value and is related to the length of minimal geodesics on the 
manifold of unitary operators that act on Hilbert space. Using the 
Euler-Arnold formalism, Balasubramanian demonstrates that there is always a 
geodesic between the identity and the time evolution operator e−iHt, whose 
length grows linearly with time. This geodesic is minimal until there is an 
obstruction to its minimality, after which it can fail to be a minimum 
either locally or globally. Balasubramanian identifies a criterion — the 
Eigenstate Complexity Hypothesis (ECH) — which bounds the overlap between 
off-diagonal energy eigenstate projectors and the k-local operators of the 
theory — and uses it to show that the linear geodesic will at least be a 
local minimum for exponential time. He shows numerically that the large-N 
SYK model (which is chaotic) satisfies ECH and thus has no local 
obstructions to linear growth of complexity for exponential time, as 
expected from holographic duality. In contrast, he also studies the case 
with N=2 fermions (which is integrable) and finds short-time linear 
complexity growth followed by oscillations. His analysis relates complexity 
to familiar properties of physical theories, like their spectra and the 
structure of energy eigenstates, and has implications for the hypothesized 
computational complexity class.
 

Christine Muschik
University of Waterloo

How to Simulate Lattice Gauge Theories on Quantum Computers

Gauge theories are fundamental to our understanding of interactions between 
the elementary constituents of matter as mediated by gauge bosons. Muschik 
will talk about proposals for quantum simulations of gauge theories and 
their recent implementation on a trapped ion quantum computer. Considering 
one-dimensional quantum electrodynamics, Muschik and collaborators 
addressed the real-time evolution of particle-antiparticle pair production 
in a digital quantum simulation [Nature 534, 516-519 (2016)] as well as 
hybrid classical-quantum algorithms [Nature 569, 355 (2019)] to simulate 
equilibrium problems. Muschik will also discuss recent results on extending 
this work beyond one spatial dimension.
 

Alex Maloney
McGill University

De Sitter Quantum Gravity in 2 and 3 Dimensions

Maloney will discuss aspects of JT gravity in two-dimensional nearly de 
Sitter (dS) space-time and pure de Sitter quantum gravity in three 
dimensions. Both are essentially topological theories of gravity where it 
is possible to study precisely the wave function of the universe following 
the Hartle-Hawking construction. The wave function can be computed by 
analytic continuation to Euclidean AdS, rather than the sphere; this allows 
us to compute all of the perturbative and (in two dimensions) 
nonperturbative corrections to the wave function and to formulate the 
theory as a Matrix integral and provides a connection with the quantization 
of the moduli space of Riemann surfaces.
 

Stephen Shenker
Stanford University

Black Holes, Random Matrices, Baby Universes and D-branes

The energy spectrum of generic large AdS black holes is discrete because 
their entropy is finite. The explanation for this is clear from the 
boundary field theory point of view in AdS/CFT — it is just the discrete 
spectrum of a bound quantum system. But the explanation for this 
discreteness from the bulk gravitational point of view remains a mystery. 
We will discuss some progress on a simpler related problem: the 
gravitational origin of the statistical properties of this discrete 
spectrum in an ensemble of quantum systems. Because black holes are quantum 
chaotic systems, we expect these statistics to be described by random 
matrix ensembles. Shenker’s analysis will focus on the simple model black 
hole described by the Sachdev-Ye-Kitaev (SYK) model and, in particular, on 
its low-energy limit, Jackiw-Teitelboim (JT) gravity. We will be led to 
consider an asymptotic expansion described by space-time manifolds with an 
arbitrary number of handles and its completion by an analog of D-branes. We 
will close by discussing some of the questions this analysis raises — based 
on joint work with Phil Saad and Douglas Stanford.
 

Jonathan Oppenheim
University College London

A Post-Quantum Theory of Classical Gravity?

Oppenheim presents a consistent theory of classical gravity coupled to 
quantum field theory. The dynamics are linear in the density matrix, 
completely positive and trace preserving, and reduce to Einstein’s 
equations in the classical limit. The constraints of general relativity are 
imposed as a symmetry on the equations of motion. The assumption that 
gravity is classical necessarily modifies the dynamical laws of quantum 
mechanics; the theory must be fundamentally stochastic involving 
finite-sized and probabilistic jumps in space-time and in the quantum 
field. Nonetheless, the quantum state of the system can remain pure, 
conditioned on the classical degrees of freedom. The measurement postulate 
of quantum mechanics is not needed since the interaction of the quantum 
degrees of freedom with classical space-time necessarily causes collapse of 
the wave function. More generally, Oppenheim derives a form of 
classical-quantum dynamics using a noncommuting divergence, which has as 
its limit deterministic classical Hamiltonian evolution and which doesn’t 
suffer from the pathologies of the semi-classical theory. The theory can be 
regarded as fundamental or as an effective theory of QFT in curved space 
where back-reaction is consistently accounted for.


@philipthrift

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